Abstract <p>The <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9008_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="138" /> </InlineMediaObject> <EquationSource Format="TEX">\({{e}^{ + }}{{e}^{ - }} \to {{\pi }^{ + }}{{\pi }^{ - }}2{{\pi }^{0}}\eta \)</EquationSource> <!--PhysPart2470165Botov-m3--> </InlineEquation> process was studied by using the data collected with the SND detector at the VEPP-2000 <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9008_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\({{e}^{ + }}{{e}^{ - }}\)</EquationSource> <!--PhysPart2470165Botov-m4--> </InlineEquation>-collider in 2011, 2012, and 2019–2021. The cross section of this process was measured in the center-of-mass energy region from 1.55 to 2 GeV. The cross section was fitted well by the vector dominance model (VDM) with the <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9008_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho (1700)\)</EquationSource> <!--PhysPart2470165Botov-m5--> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11496_2025_9008_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho (2150)\)</EquationSource> <!--PhysPart2470165Botov-m6--> </InlineEquation> resonances. Comparison with the only previous measurement at the BABAR detector was performed.</p>

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Measuring the \({{e}^{ + }}{{e}^{ - }} \to {{\pi }^{ + }}{{\pi }^{ - }}2{{\pi }^{0}}\eta \) Cross Section with the SND Detector

  • A. A. Botov,
  • M. N. Achasov,
  • A. Yu. Barnyakov,
  • K. I. Beloborodov,
  • A. V. Berdyugin,
  • A. G. Bogdanchikov,
  • T. V. Dimova,
  • V. P. Druzhinin,
  • V. N. Zhabin,
  • L. V. Kardapoltsev,
  • D. P. Kovrizhin,
  • A. A. Korol,
  • A. S. Kupich,
  • A. P. Kryukov,
  • N. A. Melnikova,
  • N. Yu. Muchnoy,
  • A. E. Obrazovsky,
  • E. V. Pakhtusova,
  • K. V. Pugachev,
  • S. I. Serednyakov,
  • Z. K. Silagadze,
  • I. K. Surin,
  • A. G. Kharlamov,
  • D. A. Shtol

摘要

Abstract

The \({{e}^{ + }}{{e}^{ - }} \to {{\pi }^{ + }}{{\pi }^{ - }}2{{\pi }^{0}}\eta \) process was studied by using the data collected with the SND detector at the VEPP-2000 \({{e}^{ + }}{{e}^{ - }}\) -collider in 2011, 2012, and 2019–2021. The cross section of this process was measured in the center-of-mass energy region from 1.55 to 2 GeV. The cross section was fitted well by the vector dominance model (VDM) with the \(\rho (1700)\) and \(\rho (2150)\) resonances. Comparison with the only previous measurement at the BABAR detector was performed.